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P-AH curves

Method p-AH curves was used to study the property of two-phase equilibrium for aqueous mixtmes with ethanol... [Pg.84]

C2H6O), methanol (CH4O) and acetone (CsHeO) at a constant content of water (0.5 mol.fr.) (Wormald and Vine, 2000 Wormald and Yerlett, 2000, 2002). The enthalpy increments (AH), measured with a cormter-current water-cooled flow calorimeter, were plotted as a function of pressure and represented as a set of isothermal p-AH curves. If these curves cross a two-phase region, they have two breaks at the dew and bubble point pressures, and the straight lines between them. In this way the values of the molar enthalpy of the saturated vapor and the molar enthalpy of the saturated liquid were obtained, as well as the molar enthalpy of flash vaporization of the mixtures. [Pg.85]

Next suppose AS , and AH , are both positive. In this case these two partially offset one another, and a plot of AGj resembling that shown in Fig. 8.2b may result. We are particularly interested in the two minima in this curve and the hump between them. A common tangent can always be drawn to two such minima so the above discussion shows that the minima at points P and Q in Fig. 8.2b each have the same values of AjUi and A/i2. Since AjUj is simply the difference between juj and its value for the pure component, the chemical potential for each component is seen to have the same value for both solution P and solution Q in Fig. 8.2b. [Pg.530]

Viscosity is equal to the slope of the flow curve, Tf = dr/dj. The quantity r/y is the viscosity Tj for a Newtonian Hquid and the apparent viscosity Tj for a non-Newtonian Hquid. The kinematic viscosity is the viscosity coefficient divided by the density, ly = tj/p. The fluidity is the reciprocal of the viscosity, (j) = 1/rj. The common units for viscosity, dyne seconds per square centimeter ((dyn-s)/cm ) or grams per centimeter second ((g/(cm-s)), called poise, which is usually expressed as centipoise (cP), have been replaced by the SI units of pascal seconds, ie, Pa-s and mPa-s, where 1 mPa-s = 1 cP. In the same manner the shear stress units of dynes per square centimeter, dyn/cmhave been replaced by Pascals, where 10 dyn/cm = 1 Pa, and newtons per square meter, where 1 N/m = 1 Pa. Shear rate is AH/AX, or length /time/length, so that values are given as per second (s ) in both systems. The SI units for kinematic viscosity are square centimeters per second, cm /s, ie, Stokes (St), and square millimeters per second, mm /s, ie, centistokes (cSt). Information is available for the official Society of Rheology nomenclature and units for a wide range of rheological parameters (11). [Pg.167]

Fig. 92. Mass spectral parameters pressure (p in torr) and ionic currents (J in relative units) of Li2NbOF5 (A), Na2NbOFs (B) and K2NbOFs (C) versus temperature in °C (after Agulyansky et ah, [383]). Numbers on the curves correspond to ions as shown in Fig. 91. Fig. 92. Mass spectral parameters pressure (p in torr) and ionic currents (J in relative units) of Li2NbOF5 (A), Na2NbOFs (B) and K2NbOFs (C) versus temperature in °C (after Agulyansky et ah, [383]). Numbers on the curves correspond to ions as shown in Fig. 91.
It can be seen that k in Eq. (10) replaces the system-describing parameters L and Ah in Eq. (1). A direct test of the hypothesis is therefore to plot (j> against k for fixed values of P, G, and d, with L and Ah varying. For the hypothesis to be correct, the data points must all lie on a smooth curve. Experience shows, however, that plotting (f> against k often produces an undue amount of scatter which may obscure and distort any true relationship existing. This enhanced scatter is caused by the cumulative effect of experimental errors in the various terms in the heat-balance equation from which the quality k is derived. [Pg.243]

Fig. 26. Burn-out curves for Freon-12 in uniformly heated round tubes [from Stevens et al. (SI3)]. d = 0.334 in., P = 155 psia, Ah = 0. Fig. 26. Burn-out curves for Freon-12 in uniformly heated round tubes [from Stevens et al. (SI3)]. d = 0.334 in., P = 155 psia, Ah = 0.
We are permitted to assume that dp is directly proportional to dT because AH and AV are regarded as constants, although even a casual inspection of a phase diagram shows how curved the solid-gas and liquid-gas phase boundaries are. Such curvature clearly indicates that the Clapeyron equation fails to work except over extremely limited ranges of p and T. Why ... [Pg.197]

The data in Table 8.4 [4] represent the vapor pressure of mercury as a function of temperature. Plot In P as a function of 1/T to a scale consistent with the precision of the data. If the resultant plot is linear, calculate AH Iz from the slope obtained by a least-squares fit to the line. If the plot is curved, use a numerical differentiation procedure to obtain the value of AHmjZ as a function of T, and calculate ACpm- See Appendix A for methods. [Pg.208]

Plots of log P vs 1/T for several R2C07-H systems are shown in Figures 3 and 4. The AH values, giving the heats of desorption of hydrogen from the compound, were obtained from the slopes of the curves in Figures 3 and 4 and are listed in Table II. [Pg.325]

A differentiation of the Arrhenius-plot from Fig. 18 by means of spline polynomials gives the second term of the activation enthalpy (31), whereas its first term can be calculated in the way shown in Section 3.1. The results are given in Fig. 20 for three typical degrees of polymerization. The full lines show the temperature-dependence of the activation enthalpy (31), whereas the dashed lines show the corresponding reversible contributions (10a), as predicted by Casper s approximation ( q = 0, v = 1, a = 1) of Eq. (19) of the PDC-calibration curves. The dependence of AH on the degree of polymerization P at two typical column temperatures is shown in Fig. 21 where also the P-dependence of the corresponding activation entropies (33) is plotted for comparison (dashed lines). [Pg.37]

Using the values of Tc = 253 K from 16 and AH = - 0.67 kcal per repeat unit for its model 20, AS = - 2.6 cal K-1 at Tc. Since the sign of the AG term below Tc is negative, P is more stable than M, and vice versa. To design a thermo-driven PM-transition polysilane for switching at a desired temperature, it seems to be essential that the polysilane has a double-well potential curve, small AH, and small potential barrier height. If the AS term is responsible for the inver-... [Pg.150]

Figure 1.2 Potential energy curves for the approach of a hydrogen molecule and of two hydrogen atoms to a metal surface E is the activation energy — AH is the heat of adsorption subscripts p and c are, respectively, physical adsorption and chemisorption. Figure 1.2 Potential energy curves for the approach of a hydrogen molecule and of two hydrogen atoms to a metal surface E is the activation energy — AH is the heat of adsorption subscripts p and c are, respectively, physical adsorption and chemisorption.
Consider a plot of AH, the heat of solution based on one mole of solute (species 1), vs. ft, the moles of solvent per mole of solute, at constant T and P. Figure 13.7 is an example of such a plot, except that the plot considered here has a linear rather than logarithmic scale along the abscissa. Let a tangent drawn to the AH vs. n curve intercept the ordinate at point I. [Pg.246]


See other pages where P-AH curves is mentioned: [Pg.3]    [Pg.4]    [Pg.14]    [Pg.15]    [Pg.15]    [Pg.3]    [Pg.4]    [Pg.14]    [Pg.15]    [Pg.15]    [Pg.217]    [Pg.651]    [Pg.174]    [Pg.160]    [Pg.68]    [Pg.507]    [Pg.48]    [Pg.120]    [Pg.357]    [Pg.236]    [Pg.188]    [Pg.125]    [Pg.231]    [Pg.374]    [Pg.293]    [Pg.313]    [Pg.313]    [Pg.68]    [Pg.125]    [Pg.150]    [Pg.225]    [Pg.938]    [Pg.342]    [Pg.104]    [Pg.330]    [Pg.178]    [Pg.562]    [Pg.346]    [Pg.156]    [Pg.101]    [Pg.120]   
See also in sourсe #XX -- [ Pg.4 ]




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